MICELLAR EFFECT ON THE FLUORESCENCE QUENCHING OF INDOLIC COMPOUNDS BY AMINOACIDS

Abstract— The photolysis in aqueous neutral solutions of 5-nitrofurfural (NFA), an important metabolite of nitrofurans used as medicines, was investigated. Upon UV-A irradiation NFA loses up to 70 mol % nitrite, with formation of 5-hydroxymethylene-2(5H)-furanone, a new substance. When Cl⁻¹ is present 5-chlorofurfural is an important photoproduct. Photo-induced addition of either OH or CI⁻¹, followed by thermochemical elimination of NO₂⁻¹, is the proposed mechanism. Furthermore, NFA reacts with nitrite yielding nifuroxim. The possible role of the NFA photolysis in the occurrence of (photo)biological effects of NFA is discussed.     

Three-dimensional numerical simulation of the wake flow of an afterbody at subsonic speeds

We numerically investigate the wake flow of an afterbody at low Reynolds number in the incompressible and compressible regimes. We found that, with increasing Reynolds number, the initially stable and axisymmetric base flow undergoes a first stationary bifurcation which breaks the axisymmetry and develops two parallel steady counter-rotating vortices. The critical Reynolds number (Re _cs) for the loss of the flow axisymmetry reported here is in excellent agreement with previous axisymmetric BiGlobal linear stability (BiGLS) results. As the Reynolds number increases above a second threshold, Re _co, we report a second instability defined as a three-dimensional peristaltic oscillation which modulates the vortices, similar to the sphere wake, sharing many points in common with long-wavelength symmetric Crow instability. Both the critical Reynolds number for the onset of oscillation, Re _co, and the Strouhal number of the time-periodic limit cycle, St_sat, are substantially shifted with respect to previous axisymmetric BiGLS predictions neglecting the first bifurcation. For slightly larger Reynolds numbers, the wake oscillations are stronger and vortices are shed close to the afterbody base. In the compressible regime, no fundamental changes are observed in the bifurcation process. It is shown that the steady state planar-symmetric solution is almost equal to the incompressible case and that the break of planar symmetry in the vortex shedding regime is retarded due to compressibility effects. Finally, we report the developments of a low frequency which depends on the afterbody aspect ratio, as well as on the Reynolds and on the Mach number, prior to the loss of the planar symmetry of the wake.     

The Kernel energy method: Application to graphene and extended aromatics

The quantum chemistry of finite aperiodic graphene flakes is a matter of considerable interest because of the anticipated technological importance of such objects. Since real aperiodic graphene flakes will in general be composed of many thousands of carbon atoms, theoretical methods appropriate to such large molecules would need to be used for the ab initio quantum calculation of their properties. The Kernel energy method is discussed here, and it is shown to be accurately applicable to graphenes and analogous extended aromatic molecules. It is necessary to define the kernels of a graphene molecule in a new way because of the extensive aromaticity, which defines its electronic structure. The kernels used in the reconstruction of the full graphene sheet preserve the total number of π‐electrons, Clar sextets, and the approximate overall aromaticity. Sivaramakrishnan et al. [J Phys Chem A, 2005, 109, 1621] define similar “ring conserved isodesmic reactions (RCIR).” The principal innovation of this article is the suggestion that kernels may be mathematically extracted from an extended aromatic molecule such as graphene by a fissioning of aromatic bonds. Hartree Fock (HF) and Møller‐Plesset (MP2) chemical models using a Gaussian basis of 3‐21G orbitals are used to calculate the total energy of a graphene flake. This demonstration calculation is performed on a graphene flake in which dangling bonds are saturated with hydrogens (C₇₈H₂₆) composed of a total of 104 atoms arranged in 27 benzenoid rings. The KEM with both types of chemical model are shown to be accurate to nearly 1 kcal/mol, of a total energy, which is nearly 3000 atomic units, that is, with an absolute error within “chemical accuracy” and a relative error of the order of 5 × 10⁵% of the total energy. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2011     

Photopolymerization of acrylamide initiated by the three‐component system safranine/triethanolamine/diphenyliodonium chloride: The effect of the aggregation of the salt

The effects of diphenyliodonium chloride (DPI) on the polymerization of acrylamide photoinitiated by the dye safranine with triethanolamine as a coinitiator were investigated in aqueous solutions. The salt notably increased the polymerization rate. This accelerating effects increased appreciably at concentrations of DPI at which the light scattering of the solutions became important. The effects of DPI on the photophysical properties of the dye were also investigated. Although the absorption and fluorescence were scarcely affected, the triplet yield increased by 60%. However, the polymerization rate increased by a factor much higher than that of the triplet yield. The results obtained at high concentrations of the salt could be ascribed to the presence of aggregates of the hydrophobic cations. The lower limit established for the formation of the aggregates was a DPI concentration of approximately 1 × 10⁻³ M. Possible mechanisms for the action of the salt were examined. © 2004 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 42: 4916–4920, 2004     

TWO NEW STERICALLY HINDERED PHTHALOCYANINES: SYNTHETIC AND PHOTODYNAMIC ASPECTS

The synthesis and the properties of 1,4-dibutoxy-2,3-dicyanotriptycene, of a metal-free tetradibenzobarrelenooctabutoxyphthalocyanine, and of the corresponding zinc phthalocyanine are described. The two phthalocyanines do not aggregate when dissolved in benzene at concentrations up to 450 microM. For the metal-free and the zinc compounds, the red band maxima are at 736 and 757 nm, the triplet maxima are at 590 and 605 nm, the triplet state lifetimes are 58 and 177 microseconds, and the protoporphyrin-IX dimethyl ester-to-compound bimolecular rate constants for triplet energy transfer are 2.61 x 10(8) and 1.47 x 10(8) M-1 s-1. Triplet energy transfer from the metal-free compound to O2 is endoergonic by 1.0 kcal mol-1. The potential of the zinc compound for photodynamic therapy is touched upon.     

FLUORESCENCE QUENCHING OF INDOLIC COMPOUNDS BY ALIPHATIC AMINO ACIDS. EVIDENCE FOR EXCITED STATE COMPLEXES

Abstract The fluorescence quenching of indole, tryptophan, tryptamine and indole-3-acetic by aliphatic amino acids was studied. The bimolecular rate constant ( k _q) for the deactivation of the excited state was determined. The k _q values were in the range 0.6 × 10⁸–1.6 × 10⁹ M ^–1 S^–1 and they increased in the order tryptophan < tryptamine < indole ≈ indole-3-acetic acid. When the rate constant was corrected for diffusion al effects a good linear correlation was found between the log ( k '_q) and the ionization equilibrium constant of the carboxylic group of the amino acid (p ^k _a1). This was interpreted as arising from a charge transfer mechanism in which the indole moiety acts as an electron donor and the carbonyl group of the amino acid as the acceptor.
The activation parameter for the quenching processes were also determined. The ΔH^≠ values were in the range —4.0 to +4.0 kcal/mol and the ΔH^≠ in the range –7 to –37 e.u. For the systems with lower values of k _q negative values for ΔH^≠ were observed. A good enthalpy-entropy compensation was found with an isokinetic temperature of 229 K. These results suggest that a common mechanism is operating for all the systems and that it involves the formation of an excited state complex between the indolic compound and the amino acid.     

Proton-transfer mediated quenching of pyrene/indole charge-transfer states in isooctane solutions

The fluorescence quenching of pyrene (Py) by a series of N-methyl and N-H substituted indoles was studied in isooctane at 298 K. The fluorescence quenching rate constants were evaluated by mean of steady-state and time-resolved measurements. In all cases, the quenching process involves a charge-transfer (CT) mechanism. The I(o)/I and tau(o)/tau Stern-Volmer plots obtained for the N-H indoles show a very unusual upward deviation with increasing concentration of the quenchers. This behavior is attributed to the self-quenching of the CT intermediates by the free indoles in solution. The efficiency of quenching of the polyaromatic by the N-H indoles increases abruptly in the presence of small amount of added pyridine (or propanol). A detailed analysis of the experimental data obtained in the presence of pyridine provides unambiguous evidence that the self-quenching process involves proton transfer from the CT states to indoles.     

PORPHYRIN-LIPID INTERACTIONS AT THE AIR-WATER INTERFACE IN SPREAD MONOLAYERS. A FLUORESCENCE STUDY.

In membrane systems, carboxylic porphyrins may interact with both the lipid pseudophase and the adjacent aqueous environment through their hydrophobic core and their polar acid chains, respectively. These interactions are monitored in model membrane systems, i.e. spread monolayers of dioleoylphosphatidylcholine as functions of lipid organization and pH of the aqueous subphase using steady state and time resolved fluorescence techniques. In all cases contact between porphyrin and aqueous subphase, as indicated through quenching by I^-, is observed at low surface pressure. This contact decreases and becomes almost insignificant as the monolayer approaches maximum organization through compression. On deprotonation of the monocarboxylic porphyrin, methylpyrroporphyrin, increased contact with water is observed in liquid compressed monolayers. In liquid expanded layers, however, it appears that organization of lipid molecules surrounding this dissymmetric charged form affords some isolation from water. The effect of esterification of carboxylic chains is also examined.     

Structural Characterization of Divalent Magnesium-Dopedα-Fe2O3

The defect structure of divalent magnesium-dopedα-Fe₂O₃has been examined by Rietveld structure refinement of the X-ray powder diffraction data. The results show that the Mg²⁺ions occupy the vacant interstitial octahedral sites as well as substituting on the two adjacent octahedral Fe³⁺sites in the corundum-relatedα-Fe₂O₃structure. The structure therefore involves a linear cluster of three Mg²⁺ions replacing two Fe³⁺ions. Interatomic potential calculations indicate that this is the most energetically favorable defect cluster for the system.